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No-core Monte Carlo shell-model calculation for 10Be and 12Be low-lying spectra

机译:10Be和12Be低洼光谱的无核蒙特卡洛壳模型计算

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The low-lying excited states of 10Be and 12Be are investigated within a no-core Monte Carlo shell-modeln(MCSM) framework employing a realistic potential obtained via the unitary correlation operator method. Thenexcitation energies of the 2+n1 and 2+n2 states and theB(E2; 2+n1,2n→ 0+ng.s.) value for 10Be in theMCSMwith a standardntreatment of spurious center-of-mass motion show good agreement with experimental data. Some properties ofnlow-lying states of 10Be are studied in terms of quadrupole moments,E2 transitions, and single-particle occupationnnumbers. The E2 transition probability of 10C, themirror nucleus of 10Be, is also presented with a good agreementnto experiment. The triaxial deformation of 10Be and 10C is discussed in terms of the B(E2) values. The removalnof the spurious center-of-mass motion affects various states differently: for instance, it has a negligible effect onnthe 2+n1 and 2+n2 levels of 10Be, while it leads to a significant and favorable shift for the 1−n1 level. It is suggestednthat the description of 12Be needs a larger model space as well as some other higher excited states of 10Be, as annindicator that these are dominated by intruder configurations.
机译:在无核蒙特卡洛壳模型(MCSM)框架内,利用通过correlation相关算子方法获得的真实势,研究了10Be和12Be的低激发态。然后,对MCSM中的10Be进行2 + n1和2 + n2态的激发能以及B(E2; 2 + n1,2n→0 + ng.s。)值,并用标准的假性质心运动对其进行处理,这与实验结果吻合良好。数据。根据四极矩,E2跃迁和单粒子占据数研究了10Be低态的一些性质。实验中也给出了10C的E2跃迁概率,即10Be的镜核。根据B(E2)值讨论了10Be和10C的三轴变形。虚假质心运动的去除对各种状态的影响不同:例如,它对10Be的2 + n1和2 + n2级别的影响微不足道,而导致1-n1级别的显着且有利的偏移。建议对12Be的描述需要更大的模型空间,以及10Be的其他一些更高的激发态,以指示这些状态主要受入侵者的配置影响。

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  • 来源
    《Physical Review C: Nuclear Physics》 |2012年第1期|p.1-9|共9页
  • 作者单位

    Department of Physics, University of Tokyo, Hongo, Tokyo 113-0033, Japan, and State Key Laboratory of Nuclear Physics and Technology,School of Physics, Peking University, Beijing 100871, People’s Republic of China;

    Department of Physics and Center for Nuclear Study, University of Tokyo, Hongo, Tokyo 113-0033, Japan andNational Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA;

    Department of Physics, University of Tokyo, Hongo, Tokyo 113-0033, Japan;

    Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195 Japan;

    Institut f¨ur Kernphysik, Technische Universit¨at Darmstadt, D-64289 Darmstadt, Germany;

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